Hillock formation on high-temperature annealed AlN templates due to dislocation nucleation at AlON particles

A A. Lachowski (Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,) T T. Remmele (Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,) A A. Kwasniewski (Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,) C C. Hartmann (Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,) M M. Żak (Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,) J J. Smalc-Koziorowska (Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,) M M. Petkovic (Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,) M M. Albrecht (Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,) T T. Schulz

Abstract

The origin of hillocks in AlGaN layers grown on high-temperature annealed (HTA) AlN templates has been reinvestigated. During the HTA process, AlON precipitates form within the AlN matrix due to oxygen contamination. The thermal mismatch between the precipitates and the compressively strained AlN generates shear stress on pyramidal glide planes, which provide the glide system for (a + c) dislocations. Importantly, the proximity of a precipitate to the free surface amplifies this localized shear field and lowers the barrier for half-loop formation, making subsurface precipitates the most effective dislocation sources. Once the shear stress reaches a critical value, a single (a + c) dislocation half-loop nucleates. The threading segments of the loop terminate at the HTA-AlN surface and trigger spiral growth during AlGaN epitaxy, ultimately leading to hillock formation.

Article Details

Volume / Issue Vol. 128, Issue 20
Published May 18, 2026
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (9)

A

A. Lachowski

Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,

T

T. Remmele

Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,

A

A. Kwasniewski

Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,

C

C. Hartmann

Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,

M

M. Żak

Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,

J

J. Smalc-Koziorowska

Institute of High Pressure Physics, Polish Academy of Sciences 1 , Sokolowska 29/37, 01-142 Warsaw,

M

M. Petkovic

Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,

M

M. Albrecht

Leibniz-Institut für Kristallzüchtung 2 , Max-Born Str. 2, 12489 Berlin,

T

T. Schulz